2002
DOI: 10.1002/1521-3765(20020415)8:8<1785::aid-chem1785>3.0.co;2-x
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Electronic Properties of the Silver–Silver Chloride Cluster Interface

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Cited by 88 publications
(69 citation statements)
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References 32 publications
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“…The vibrational energy will be dissipated via anharmonicity into lattice phonons, and the lattice will reach the new equilibrium position Q 2 , i.e., the relaxed excited state. After the mean lifetime has elapsed, the excited electron returns by a vertical emission process to the ground state, and the subsequent lattice relaxation completes the optical cycle [5][6][7][8]. To construct the configuration coordinate diagrams, the ion clusters representing the F A1 :Ga + , F A1 :Au + , F A1 :Ca 2+ , and F A1 :Sr 2+ centers on the (100) surfaces of LiCl were first embedded into the three-dimensional arrays of the point ions described in the "Surface simulation" section.…”
Section: Configuration Coordinate Diagramssupporting
confidence: 78%
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“…The vibrational energy will be dissipated via anharmonicity into lattice phonons, and the lattice will reach the new equilibrium position Q 2 , i.e., the relaxed excited state. After the mean lifetime has elapsed, the excited electron returns by a vertical emission process to the ground state, and the subsequent lattice relaxation completes the optical cycle [5][6][7][8]. To construct the configuration coordinate diagrams, the ion clusters representing the F A1 :Ga + , F A1 :Au + , F A1 :Ca 2+ , and F A1 :Sr 2+ centers on the (100) surfaces of LiCl were first embedded into the three-dimensional arrays of the point ions described in the "Surface simulation" section.…”
Section: Configuration Coordinate Diagramssupporting
confidence: 78%
“…After the emission process, the assumed saddle-point ion has a 50% chance of hopping to the <110> anion vacancy site opposite its starting location. Therefore, if the F A center system is excited in either one of its absorption bands by polarized light with a direction of propagation parallel to the <100> axis and its electric field vector E parallel to the perpendicular <100> axis, the F A centers excited by this E vector will quickly be reoriented to the <100> direction, at which point the F A centers will no longer be excited, and this reoriented system will become experimentally transparent for the excitation light [5][6][7][8]. However, it has been observed experimentally and theoretically by many workers that no spectral region in the absorption range of the F A band is completely transparent, even after prolonged preferential optical excitation of the F A centers.…”
Section: Orientational Destructionmentioning
confidence: 96%
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“…Additional AgCl surface states (SURS), as well as metal induced gap states (MIGS) from Ag/AgCl cluster composites also present in the bandgap region of silver chloride. These different levels are responsible for the self-sensitization of silver chloride [77,78]. They allow excitation of electrons, hence, creation of holes in the valence band by light absorption below bandgap energy.…”
Section: Photocatalytic and Photoelectrochemical Water Splittingmentioning
confidence: 99%
“…Microorganisms with resistance to the antimicrobial activity of Ag are exceedingly rare. Such silver has a size of nano-level, the total surface area of the silver become larger in identity volume and antibacterial efficiency is increased (Glaus et al, 2002;Rujitanaroj et al, 2008). PVA is a semi-crystalline hydrophilic polymer with good chemical and thermal stability.…”
Section: Introductionmentioning
confidence: 99%